Making cold molecules from cold atoms
Photoassociation (AB)* Ground state A + B Photoassociation is resonant in the photon energy Usually achieved by adding an extra laser to a MOT – the PA laser Very little heating involved – the molecules are ultracold Molecules will be in low-lying rotational states Produces molecules in highly excited vibrational states
Photoassociation – decay channels Decay to free atoms Decay to bound state Ground state A + B (AB)*
Photoassociation properties Occurs at outer turning point of excited vibrational state Extremely inefficient for tightly bound states – tend to form “long-range molecules” Decay to a deeply bound state of the molecular ground state is unlikely Decay to two free atoms is accompanied by a large release of energy – trap loss Li2, Na2, K2, Rb2, Cs2, Sr2 , Ca2 , LiCs....
Detection methods PRL 85, 2292 (2000) Trap loss spectroscopy – the number of atoms in a MOT decreases when the molecules are formed. Example below: Ca2 Rev. Mod. Phys. 78, 483 (2006) Ion detection. Ionize the molecules and count the ions produced.
Example: production of ultracold LiCs in the ground state Photoassociation into v=4 (500mW, 946nm) Spontaneous decay into ground state Two-photon resonant ionization PRL 101, 103004 (2008) 5000 ground state molecules per second
Photoassociation - advantages and limitations Molecules are formed at ultracold temperatures Possible to reach the ground state (though difficult) Limited to constituents that can be laser-cooled High experimental complexity, particularly for heteronuclears Production rate is usually very slow
Feshbach resonance
Reminder about s-wave scattering At ultracold temperatures, scattering is described by the s-wave scattering length, a All other partial waves are suppressed by the angular momentum barrier Toy example: V=∞ V=V0 V=0 Zero-energy scattering state Uppermost bound state u(R) exp(-R/a) u(R) (R – a)
Feshbach resonance
Reminder about level crossings
Atoms into molecules via a Feshbach resonance B / B0 Bound molecules Free atoms